Neutronic reactor



Sept 15 1953 E. FERMI Erm. 2,852,461

` NEUTRONIC REACTOR Filed oct. 11, 1945 FIEL PIE- Z.

a JJHJVJZ@ Maf tz/orne! NEUTRoNIC nEAcTon Enrico Fermi, Santa Fe, N. Mex., Walter H. Zinn, Chicago, Ill., and Herbert L. Anderson, Hartford, Conn., Vassi'gnors to the United States of America as represented by the United States Atomic Energy Commission Application October 11, 1945, Serial No. 621,337

1 Claim. (Cl. 204193.2)

This invention relates to the general subject of nuclear fission, and more particularly to a novel means for imu proving the establishment of self-sustaining nuclear fission chain reactions.

In order to attain a self-sustaining chain reaction in a system of practical size, the ratio of the number of neutrons produced in one generation by the lissions, to the original number of neutrons initiating the fissions, must be known to be greater than unity after all neutron losses are deducted, and this ratio is, of course, dependent upon the values of the pertinent constants.

In a self-sustaining chain reaction of uranium with slow neutrons, as presently understood, 92238is converted by neutron capture to the isotope 92229. AThe latte'r is converted by beta decay to 93239 and `this 93239 in turn is converted by beta decay to 94235. Other isotopes of 93 and 94 may 4be formed in small quantities. By slow or thermal neutron capture, 92225 on the other hand, can undergo nuclear fission to release energy pearing as heat, gamma and beta radiation, together with the formation of fission fragments appearing as radio active isotopes of elements of lower mass numbers, and with the release ot' secondary neutrons.

The secondary neutrons thus produced by the iissioning of the 92235 nuclei have a high average energy, and inust be slowed down to thermal energies iii-order to be i'n condition to cause slow neutron fission in other 92225 nuclei. This `slowing down, or moderation of the neutron energy, is accomplished by passing the neutrons through a material Where the neutrons are slowed by collision. Such a material is known as a moderator. While some of the secondary neutrons are absorbed by the uranium isotope 92238 leading to the production ot element 94, and by other materials such as the moderator, enough neutrons can remain to sustain the chain reaction when proper conditions are maintained.

Under these properconditions, the chain reaction will supply not only the neutrons necessary iormaintaining the neutronic reaction, but also will supply the neutrons for capture by the isotope 92238 leading to the production of 94, and excess neutrons lor use dos ed.

As 94 is a transuranic element, it can separated. from the unconverted uranium by chemical meth-cds, und as it is issionable by slow neutrons in Va manner similar to the isotope 92235, it is valuable, for example, for enriching natural uranium for use in other chain reacting s'ystems of smaller overall size. The fission frag ments are also valuable as sources of radioactivity. l

The ratio of the fast neutrons produced in one generation .by the issions to the original number of fast neutrons in a theoretical system of iminite size where there can be no external loss of neutrons is called the reproduction or multiplication factor or constant or", the system, and is denoted by the symbol K. For any nite system, some neutrons will escape from the periphery of the system. Consequently a system of finite size may be said to have a it'. constant, even though the value Patented Sept. 16, 1958 2 thereof would only exist if the system as built were extended to infinity without change of geometry or materials.

Thus when K is referred to herein as a constant of a system of practical size, it always refers to what would exist in the same type of system of infinite size. lf K can be made suliciently greater than Unity to indicate a net gain in neutrons in the theoretical system of innite size, and then an actual system is built to be suiciently large so that this gain is not entirely lost by leakage -from the exterior surface of the system, then a self-sustaining chain reacting system of finite and practical size can be built to produce power and related byproducts by nuclear lission of natural uranium. The neutron reproduction ratio in a system of finite size therefore, differs from K by the external leakage factor, and by a factor due to the neutron absorption by localized neutron absorbers; and the reproduction ratio must still .be greater than unity to permit the neutron density to rise exponentially with time in the system as built.

More specific details of the theory and of the essential characteristics of vneutronic reactors `and neutronic reactor systems are set forth in the copending applica tion of Enrico Fermi and Leo Szilard, Serial No. 568,904, filed December 19, 1944, .now Patent No. 2,708,656, dated' May 17, 1955.

During the interchange of neutrons vin va system of finite size, comprising bodies of any size disposed in a neutron moderator, neutrons may be lost to the chain reaction in -four ways:

V(1) By absorptioncr capture in the uranium con-V tent `of the bodies without producing ssion;

(2) By absorption'or capture in` the moderator material itself;

(3) By absorption or capture bythe impurities presentv in both the uranium bodies and the moderator;

(4) By leakage out of the system through the periphery thereof. A

The present invention is directed to a novel means and method for increasing the reproduction `ratio of Aa 'finite system by diminishing the nent-ron loss due to the third factor above listed, namely, impurities within the reactor.

The eiect Vof impurities on the optimum reproduction factor K may be conveniently evaluated 'by means of certain constants known as danger coe'flicients `which are assigned to the various elements. These danger c'oecients for the impurities are each multiplied by the p'rcent by weight of the corresponding impurity, with respect to the weight of Vuranium inthe system, and the "total sum of these cofricients gives a value known as the total danger sum. This total danger sum is subtracted from the reproduction constant `K as calculated for theoretical- 1y pure materials and for the -speciiic 'geometry/under c'onsideration. p 1 l The danger coecientsare deiinedin -termsof the ratio ofthe Weight of impurity per unit mass of uranium Vand are based on` the cross section `for absorption of neutrons of the various elements. These values `may be obtained from published literature on the, subject, and bywdireet measurement, and the danger coetiicient computed by' the formula l t no Tu Ai s o 3 and the result will be suiciently accurate for design purposes. n

Danger coeicients for some elements are given in the following table, wherein the elements are listed in order The sum of the danger coeflicients of the impurities in any given composition entering into a reactor as multiplied by the fraction by weight of the uranium in the reactor, is known as total danger sum of the composition. This figure is a dimensionless constant like K and accordingly can be directly subtracted from K. The danger coefficients givenV are related to a neutron absorption value of unity for uranium.V

As a specific example of the use of danger coeicients, if the materials of a system under consideration have 0.01 percent by weight of each of the elements Co, Ag and N kwith respect to the Weight of the uranium in the system, then the total danger sum in K units for such an analysis would be: Y

.000l 17-l.000l' 12H-.0001 4=.0039 This ligure can then beV sutractedrffrom the K calculation for a particular geometry of theoretically pure materials to give the actual K constant for the materials used. Y :j Y Y `rI'herefore, a' principal object ofthe present invention is-toV reduce the total danger sum Yof the impurities in a neutronic reactor bythe novel method of and means for accompariying drawing, in which:A

T-'Figg-l'is' 'a perspective view of areactor incorporating japreferred embodiment of the presenfinvention, parts n being broken away and parts being shownin ,section for clarity?. i f V i Fig. 2 is an enlarged section partly in elevation, on

Vthe line 2-7-2 of Fig. 1, taken as indicated;

Fig. 3 is an enlargedfsection partly in elevation, on the line 3--3 of Fig. 2, taken as indicated; and

Fig. 4 is a section on the line 4-4 of Fig. 3. Describing vtheginvention in detail, and referring. rst to Fig. l,` on a concrete foundationz is provided an up- -standingconcrete vault or shield 4 receiving therewithin a'neutronic reactor or pi1e,"generally designated 6, said Y reactor 6 Vbeing per se Vno parti of the present invention', n

Vformed of graphite blocks, or the like.

Vas steel.

- inwardly and outwardly of the reactor 6, thereby contro v '4 n l cation, Serial No. 568,904, tiled December 19, 1944, now Patent No. 2,708,656, dated May 17, 1955, in the joint names of Enrico Fermi and Leo Szilard. The reactor 6 shown is constructed as a lattice of uranium-containing slugs or lumps in a moderating material, such as graphite formed as blocks. Around the moderator is a reector 8 A fluid-tight casing or envelope 10 Vis disposed around the fourv sides, top, and bottom of the reflector 3 S0. that the entire reactor 6 is contained Within the casing 10, which is preferably Vformed of balloon cloth but may be constructed of any other suitable materiaLs'uch ln this connection, it may be noted that the casing 10 is preferably formed of material which is sub,- stantially neutron pervious or, in other words, material having a negligible neutron absorption, inasmuch as a neutron absorbent material, after operationv of the pile, would become highly radioactive, thereby constituting a serious hazard to operating personnel. The casingltl may enclose the vault 4 and be anchored to the found tion 2 if preferable. A suitable valve 12 is provided f evacuation ofthe casing 10. A V,

The casing 10 is clamped between a clamping rin 16 and a plate 18 (Fig. 2) by means of stud bolts '20l which extend through the plate 18 and into the freiiect 8. The plate 18 is inset into the rellectorv 8 to provide an even surface for the casing 10. Three-rods 22,12 and 2f!- of neutron absorbentmaterial, preferablyfca mium, extend into slots within the reactor 6 throng openings in the plate .i8 and the casingl 10, each of sa openings being scaled by aggland 26,'(Figs. 3l and. clamped to the plate 1S by a rectangular frame `28, vlu is secured to the plate 1S by stud bolts. A Wilson seal, I which is well-known in the art, may be employed instead of the seal just'described. n i

The rods 23 and 24 may function as safety rodsfand al l connected to suitable actuating means (notV shown) (for urging them to their innermost positions within the-r actor 6, thereby reducing lthe reproduction ratio thereof, to a value below unity, whenever'the reactor attainsa temperature of predetermined maximum value as theresult of the neutron density within the reactor.. ,T11-e rod` 22 may function as a controlV rod connected to a suitable actuating means (not shown) for moving rsaid rod 22 ling the reproduction ratio thereof kfor the purpos'eof regulating the neutron density within the reactor: Hence, ythe rods 22, 23, and 24 must 'oe able to be nio Y into and out of the reactor 6. Concrete blocksl l?. placed against the open wall and on top of the reactory The valve 1?. includes a stem of sullicicnt length'to eX-Q tend through the blocks 14. Those blocks 1.4 covering the ring 16 are recessed to4 receive the ring 16Vand'stutlsf 20.y l

In constructing the above-described system embodying the present invention, the blocks of the reactor 6 includ-.fing those of the reflector 3 are piled or stackedV within the vault 4 on the casing 10. Certain of the b1ocksare,4 of course, slottedl to provide horizontal passages'througli the reactor 6 fortne reception of the rods 221, Zfand 24, During construction of the reactor 6 within the ca ing 10, lthe rods 22, 23, and 24 are inserted throughpr vided slots in the casing 10 and into the respective'y Slo in the reactor 6 as soon as that part offthe'reactorY containing the rod slots is completed. Each .rod seal completed so that the rods may be used as vcontrols in the remaining construction of the react-or 6. v 'fg After the reactor 6 is completed, the casing Altl'js servedA or otherwise sealed. The concrete blocks 14 are placed as shown, completing the vault 4. The casing, ltllisV evacuated through the valve 12, thereby reducing the A1 purities in the reactor 6, and improving the reproduction ratio thereof. Manifestly, the reproduction ratio of Vth reactor 6 may be varied by the present invention within the two extremes of an evacuated state `and of a state of air saturation. Thus, the present invention is a delicate control within such limits.

It is to be noted that a simple form of reactor 6 is illustrated and described in this application. However, it will be readily understood by `any one skilled in the art that the present invention can be utilized with other types of reactors.

It will be understood that, if desired, the reactor 6 may be built up to a point at which the reproduction ratio thereof is equivalent to unity or a value slightly lower than unity, with the control and safety rods withdrawn to their outermost positions, provided that the substantial removal of atmosphere from the reactor 6 is sufficient to raise said ratio to a value greater than unity. Then, by evacuating thecasing 10 an operative system may be obtained. However, such a practice is generally impractical because of the close tolerances involved, and in most cases it is preferable to build the reactor 6 to a size at which its reproduction ratio is greater than unity, with the control rods removed, even though the chamber is not evacuated. By atmospheric air is meant the usual atmospheric gases containing oxygen, nitrogen, and commonly a small amount of argon.

The enormous forces brought into play by the evacuation of a large neutronic reactor system or pile present problems of design resulting in involved structural forms. Furthermore, it is dilcult to make gas tight. It is better to displace the air by a non-reactive gas, that is nonreactive from both a chemical and nuclear standpoint. Suitable gases are helium and carbon dioxide. This also has the advantage of increasing K of the pile.

Other advantages of this invention include the removal from the reactor of argon which, if it remains, becomes radioactive, diffuses out of the reactor, and thus constitutes a health hazard to the operators. In addition, the removal of the oxygen in the air prevents oxidation of component parts of the reactor such as the uranium or container for the uranium.

While the theory of the nuclear chain fission reaction set forth herein is based on the best presently known experimental evidence, the present invention is not limited thereto, except by the scope of the claims, inasmuch as additional experimental data later discovered may modify the theory disclosed and other means and methods for practicing this invention within the scope of the claims may be later developed by those skilled in the art.

What is claimed is:

A neutron chain reacting device comprising a rectangular shaped neutronic reactor containing uranium disposed within a graphite block moderator and surrounded by a graphite block reflector, said reactor having a plurality of parallel adjacent slots extending therein from one surface thereof, a fluid-tight casing disposed about the reactor having an aperture therein confronting each slot in the reactor, a flat recess in the reactor confronting the apertures in the casing, a plate disposed in the recess abutting the reactor and the casing, the plate having orices therein aligned with the slots and apertures, a retaining ring disposed about the slots on the side of the casing opposite the plate and secured to the reactor to support the casing, a neutron absorbing control rod slidably disposed in each slot of the reactor and extending outwardly therefrom through the confronting orifice in the plate and aperture in the casing, a gland having an opening disposed about each control rod in contact with the surface of the casing opposite the plate,

' a frame disposed about each control rod in contact with the surface of the gland opposite the casing, a plurality of stud bolts extending through each frame and gland and anchored in the plate, and means for removing atmospheric air from the reactor.

References Cited in the le of this patent UNITED STATES PATENTS Re. 21,781 Toulmin Apr. 22, 1941 1,306,568 Weintraub June 10, 1919 2,127,193 Toulmin Aug. 16, 1938 2,205,854 Kroll .Tune 25, 1940 2,708,656 Fermi et al May 17, 1955 FOREIGN PATENTS 114,150 Australia May 2, 1940 114,151 Australia May 3, 1940 233,011 Switzerland Oct. 2, 1944 861,390 France Oct. 28, 1940 OTHER REFERENCES Smyth: Atomic Energy for Military Purposes, pp. 177-181, 70, 82-87, August 1945. Copy may be purchased from Supt. of Documents, Washington 25, D. C.

The Merriam-Webster Pocket Dictionary, p. 123, Pocket Books, Inc., N. Y. (1947), 

